The previous post described EM resonances internal to a conducting sphere. The complementary exterior problem results in scattering of EM waves off of a conducting sphere. This is known as Mie scattering and the solutions and equations are not simple (the scattered waves are combinations of reflections from the front with resonant "creeping waves" that travel over the spherical surface). However resonances begin when [tex]ka = 1[/tex], where [tex]ka[/tex] is the circumference of the sphere measured in wavelengths.
You can find the mathematical details in Jackson, Classical Electrodynamics, 2nd ed., section 9.13. The plot of how the scattering amplitude changes with circumference is found in every discussion of radar scattering cross section. See, e.g., Fig. 7 in
http://www.tscm.com/rcs.pdf"